TWI616641B - Method for measuring wafer thickness using near infrared ray - Google Patents

Method for measuring wafer thickness using near infrared ray Download PDF

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TWI616641B
TWI616641B TW106106079A TW106106079A TWI616641B TW I616641 B TWI616641 B TW I616641B TW 106106079 A TW106106079 A TW 106106079A TW 106106079 A TW106106079 A TW 106106079A TW I616641 B TWI616641 B TW I616641B
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wafer
thickness
distance
infrared light
transparent layer
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TW201831860A (en
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Qing-Fen Gao
jian-ye Wang
Wei-Qing Shao
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Abstract

一種運用近紅外線量測晶圓厚度之方法,係晶圓的上方和下方有二測頭,並虛擬一基準平面,晶圓之上、下表面皆不為近紅外線光所能穿透,由二測頭之發射器發射近紅外線光,且由對應之接收器接收反射之近紅外線光,經計算而獲得和基準平面間最遠者之距離為一第一距離,和基準平面間最近者之距離為一第二距離。透明層之厚度由其內表面所貼合之上表面或下表面及其外表面分別和基準平面間之距離的差所獲得,以第一距離減去第二距離而獲得晶圓包含透明層之總厚度,再以總厚度減去透明層之厚度而獲得晶圓本身之厚度,藉此構成本發明。A method for measuring the thickness of a wafer by using near-infrared light. There are two probes above and below the wafer, and a reference plane is virtualized. The upper and lower surfaces of the wafer are not penetrated by near-infrared light. The transmitter of the probe emits near-infrared light, and the reflected near-infrared light is received by the corresponding receiver, and the distance between the farthest distance from the reference plane is calculated to be a first distance, and the closest distance between the reference planes For a second distance. The thickness of the transparent layer is obtained by the difference between the distance between the upper surface or the lower surface of the inner surface and the outer surface thereof and the reference plane, and the second distance is subtracted from the first distance to obtain the transparent layer of the wafer. The total thickness is obtained by subtracting the thickness of the transparent layer from the total thickness to obtain the thickness of the wafer itself, thereby constituting the present invention.

Description

運用近紅外線量測晶圓厚度之方法Method for measuring wafer thickness using near infrared ray

本發明係有關一種量測晶圓厚度的技術,尤指一種運用近紅外線量測晶圓厚度之方法。 The present invention relates to a technique for measuring the thickness of a wafer, and more particularly to a method for measuring the thickness of a wafer using near infrared ray.

依中華民國專利公告號第I426574號發明專利案,揭露有光波帶經測量頭(13)沿箭頭方向(A)以非接觸方式照射到位於旋轉式固定裝置(6)上的半導體晶圓(4),反射輻射(16)則沿箭頭方向(B)被傳遞給光譜儀(17),經分析後以測得晶圓的厚度。又依中華民國專利公告號第393576號發明專利案,如其圖16(I)所示之2層磊晶晶圓內之紅外線反射之概念說明圖,同樣用以測得晶圓的厚度。然而,若前述二專利案之晶圓的表面在磊晶過程形成有金屬表面者,以紅外線光而言,由於對金屬並沒有良好的穿透性,故僅能測得金屬表面以上之表層厚度,無法測得金屬表面以下之深層厚度。 According to the invention patent of Patent No. I426574 of the Republic of China, it is disclosed that the optical wave band is irradiated to the semiconductor wafer on the rotary fixing device (6) in a non-contact manner in the direction of the arrow (A) via the measuring head (13) (4) The reflected radiation (16) is transmitted to the spectrometer (17) in the direction of the arrow (B) and analyzed to determine the thickness of the wafer. According to the invention patent of No. 393576 of the Republic of China, the concept of infrared reflection in the two-layer epitaxial wafer shown in Fig. 16(I) is also used to measure the thickness of the wafer. However, if the surface of the wafer of the above two patents is formed with a metal surface during the epitaxial process, in terms of infrared light, since the metal does not have good penetration, only the surface thickness of the metal surface can be measured. The depth of the layer below the metal surface cannot be measured.

又依中華民國專利公告號第M502953號新型專利案,揭露二電波測距器(41、42)分別照射電波於晶圓(10)的上方和下方,其反射波將由二電波測距器(41、42)所接收,應用發射電波與反射波之間的關係,可以得知二電波測距器(41、42)與晶圓(10)上方和下方的距離。將二電波 測距器(41、42)之間的距離減去由上述所量測的兩個反射波的距離即得到晶圓的厚度。然而,雖此測量裝置可測得晶圓的正確厚度,惟依實務經驗可知,所述的厚度應為總厚度,若晶圓包含有其他層結構,例如膠帶層或表面鍍膜層時,則無法從該新型專利案得知如何精確的測得晶圓本身的厚度。 According to the new patent case No. M502953 of the Republic of China Patent Publication No. M502953, it is disclosed that the two-wave range finder (41, 42) respectively illuminate the upper and lower sides of the wafer (10), and the reflected wave will be determined by the two-wave range finder (41). 42) Received, applying the relationship between the transmitted wave and the reflected wave, the distance between the second wave range finder (41, 42) and the wafer (10) can be known. Two waves The distance between the distance measuring devices (41, 42) minus the distance between the two reflected waves measured above gives the thickness of the wafer. However, although the measuring device can measure the correct thickness of the wafer, it is known from practical experience that the thickness should be the total thickness. If the wafer contains other layer structures, such as a tape layer or a surface coating layer, It is known from the novel patent how to accurately measure the thickness of the wafer itself.

因此,如何解決上述習知量測晶圓厚度之問題者,即為本發明之重點所在。 Therefore, how to solve the above problem of measuring the thickness of the wafer is the focus of the present invention.

本發明之主要目的,在於解決上述的問題而提供一種運用近紅外線量測晶圓厚度之方法,除了可透過計算而獲得晶圓包含透明層之總厚度之外,並可獲得晶圓本身之厚度,具有量測晶圓厚度之精確性和便利性。 The main object of the present invention is to solve the above problems and provide a method for measuring the thickness of a wafer by using near infrared ray, except that the total thickness of the wafer including the transparent layer can be obtained by calculation, and the thickness of the wafer itself can be obtained. It has the accuracy and convenience of measuring wafer thickness.

前述晶圓以水平設置而有一上表面和一下表面,該上表面和該下表面皆不為近紅外線光所能穿透,且該上表面和該下表面之至少一者有透明層,所述透明層有一和該上表面或該下表面貼合之內表面,且有一背對該內表面之外表面。為達前述之目的,本發明之方法,係包括以下步驟:設置測頭:有二測頭分別設在該晶圓的上方和下方,該二測頭各有一組對應的發射器和接收器,該二測頭之發射器可分別對該晶圓之上表面和下表面發射近紅外線光,且由對應之接收器接收反射之近紅外線光; 基準平面設定:該二測頭設置定位後,由該二測頭本身虛擬一位在該晶圓上或下之基準平面;量測:該二測頭之發射器分別對該晶圓之上、下表面發射近紅外線光,且由對應之接收器分別接收從該上、下表面反射之近紅外線光;前述近紅外線光遇有所述透明層時穿透,且在所述透明層之內表面所貼合之該上表面或該下表面及其外表面,皆有反射之近紅外線光被對應之接收器所接收;計算:有一計算單元和該二測頭電性連接,該晶圓之上表面和下表面以及所述透明層之外表面中,依前述各接收器所接收之近紅外線光經計算而獲得和該基準平面間最遠者之距離為一第一距離,和該基準平面間最近者之距離為一第二距離,所述透明層之厚度由其內表面所貼合之該上表面或該下表面及其外表面分別和該基準平面間之距離的差所獲得,以該第一距離減去該第二距離而獲得該晶圓包含該至少一透明層之總厚度,再以該總厚度減去該至少一透明層之厚度而獲得該晶圓本身之厚度。 The wafer is horizontally disposed to have an upper surface and a lower surface, the upper surface and the lower surface are not transparent to near-infrared light, and at least one of the upper surface and the lower surface has a transparent layer. The transparent layer has an inner surface that conforms to the upper surface or the lower surface and has a surface that faces away from the inner surface. For the foregoing purposes, the method of the present invention comprises the steps of: providing a probe: two probes are respectively disposed above and below the wafer, and each of the two probes has a corresponding set of transmitters and receivers. The emitter of the two probes respectively emit near-infrared light to the upper surface and the lower surface of the wafer, and the reflected near-infrared light is received by the corresponding receiver; The reference plane setting: after the two probes are positioned, the two probes themselves virtualize a reference plane on or under the wafer; the measurement: the transmitters of the two probes are respectively on the wafer, The lower surface emits near-infrared light, and the near-infrared light reflected from the upper and lower surfaces is respectively received by the corresponding receiver; the near-infrared light penetrates when the transparent layer is encountered, and the inner surface of the transparent layer The upper surface or the lower surface and the outer surface of the attached surface are reflected by the near-infrared light; the calculation: a computing unit and the two probes are electrically connected to the wafer In the outer surface of the surface and the lower surface and the transparent layer, the distance between the farthest infrared light received by each of the receivers and the farthest distance between the reference planes is calculated as a first distance, and the reference plane The closest distance is a second distance, and the thickness of the transparent layer is obtained by the difference between the upper surface of the inner surface or the lower surface and the outer surface thereof, and the distance between the reference plane and the reference plane, respectively. First distance minus the first It is obtained from the total thickness of the wafer comprising at least one layer of transparent, then subtracting the thickness of the total thickness of the at least one transparent layer of a thickness of the wafer obtained by itself.

其中,所述至少一透明層,有一在該晶圓之下表面的膠帶層。 Wherein the at least one transparent layer has a layer of tape on a lower surface of the wafer.

其中,所述至少一透明層,另有一在該晶圓之上表面的保護層。 Wherein the at least one transparent layer has a protective layer on the upper surface of the wafer.

其中,各該測頭之發射器所發射之近紅外線光的波長為850nm。 Wherein, the wavelength of the near-infrared light emitted by the emitter of each of the probes is 850 nm.

其中,該總厚度之量測範圍在50um至2000um。 Wherein, the total thickness is measured in the range of 50 um to 2000 um.

本發明之上述及其他目的與優點,不難從下述所選用實施例之詳細說明與附圖中,獲得深入了解。 The above and other objects and advantages of the present invention will be readily understood from

當然,本發明在某些另件上,或另件之安排上容許有所不同,但所選用之實施例,則於本說明書中,予以詳細說明,並於附圖中展示其構造。 Of course, the invention may be varied on certain components, or in the arrangement of the components, but the selected embodiments are described in detail in the specification and their construction is shown in the drawings.

1‧‧‧方法 1‧‧‧ method

11‧‧‧設置測頭 11‧‧‧Set the probe

12‧‧‧基準平面設定 12‧‧‧Base plane setting

13‧‧‧量測 13‧‧‧Measure

14‧‧‧計算 14‧‧‧ Calculation

2‧‧‧晶圓 2‧‧‧ wafer

21‧‧‧上表面 21‧‧‧ upper surface

22‧‧‧下表面 22‧‧‧ Lower surface

3‧‧‧測頭 3‧‧‧ probe

31‧‧‧發射器 31‧‧‧transmitter

32‧‧‧接收器 32‧‧‧ Receiver

4‧‧‧計算單元 4‧‧‧Computation unit

5‧‧‧膠帶層 5‧‧‧ Tape layer

51‧‧‧內表面 51‧‧‧ inner surface

52‧‧‧外表面 52‧‧‧ outer surface

6‧‧‧保護層 6‧‧‧Protective layer

61‧‧‧內表面 61‧‧‧ inner surface

62‧‧‧外表面 62‧‧‧ outer surface

R‧‧‧基準平面 R‧‧‧ reference plane

D1‧‧‧第一距離 D1‧‧‧First distance

D2‧‧‧第二距離 D2‧‧‧Second distance

D3‧‧‧第三距離 D3‧‧‧ third distance

T‧‧‧總厚度 T‧‧‧ total thickness

T1‧‧‧厚度 T1‧‧‧ thickness

T2‧‧‧厚度 T2‧‧‧ thickness

d1‧‧‧第一距離 D1‧‧‧first distance

d2‧‧‧第二距離 D2‧‧‧Second distance

d3‧‧‧第三距離 D3‧‧‧ third distance

d4‧‧‧第四距離 D4‧‧‧fourth distance

t‧‧‧總厚度 T‧‧‧ total thickness

t1‧‧‧厚度 T1‧‧‧ thickness

t2‧‧‧厚度 T2‧‧‧ thickness

t3‧‧‧厚度 T3‧‧‧ thickness

第1圖係本發明之方法的步驟流程圖。 Figure 1 is a flow chart showing the steps of the method of the present invention.

第2圖係本發明之一較佳實施例在晶圓之下表面有膠帶層者,以及二測頭量測厚度時之狀態圖。 Figure 2 is a state diagram of a preferred embodiment of the present invention with a tape layer on the underside of the wafer and a thickness measured by the two probes.

第3圖係本發明之二測頭和計算單元電性連接之方塊圖。 Figure 3 is a block diagram showing the electrical connection of the two probes and the computing unit of the present invention.

第4圖係本發明之另一較佳實施例在晶圓之下表面和上表面分別有膠帶層和保護層者,以及二測頭量測厚度時之狀態圖。 Fig. 4 is a view showing a state in which a tape layer and a protective layer are respectively provided on the lower surface and the upper surface of the wafer, and a thickness measured by the two probes in another preferred embodiment of the present invention.

請參閱第1圖至第4圖,圖中所示者為本發明所選用之實施例結構,此僅供說明之用,在專利申請上並不受此種結構之限制。 Referring to Figures 1 through 4, the structure of the embodiment selected for use in the present invention is for illustrative purposes only and is not limited by such structure in the patent application.

本發明提供一種運用近紅外線量測晶圓厚度之方法1,其係如第1圖所示,包括設置測頭11、基準平面設定12、量測13和計算14之步驟,其中: The present invention provides a method 1 for measuring the thickness of a wafer using near infrared ray, which is shown in FIG. 1 and includes the steps of providing a probe 11, a reference plane setting 12, a measurement 13 and a calculation 14, wherein:

如第2圖所示,所述晶圓2係以水平設置而有一上表面21和一下表面22,上表面21和下表面22皆不為近紅外線光所能穿透,且上表面 21和下表面22之至少一者有透明層,所述透明層有一和上表面21或下表面22貼合之內表面,且有一背對該內表面之外表面。 As shown in FIG. 2, the wafer 2 is horizontally disposed to have an upper surface 21 and a lower surface 22, and the upper surface 21 and the lower surface 22 are not penetrated by near-infrared light, and the upper surface is At least one of 21 and lower surface 22 has a transparent layer having an inner surface that conforms to upper surface 21 or lower surface 22 and has an outer surface that faces away from the inner surface.

設置測頭11:如第2圖及第3圖所示,有二測頭3分別設在晶圓2的上方和下方,二測頭3各有一組對應的發射器31和接收器32,二測頭3之發射器31可分別對晶圓2之上表面21和下表面22發射近紅外線光,且由對應之接收器32接收反射之近紅外線光。 Setting up the probe 11: As shown in FIG. 2 and FIG. 3, two probes 3 are respectively disposed above and below the wafer 2, and the two probes 3 each have a corresponding set of transmitters 31 and receivers 32, The emitter 31 of the probe 3 can emit near-infrared light to the upper surface 21 and the lower surface 22 of the wafer 2, respectively, and receive the reflected near-infrared light by the corresponding receiver 32.

基準平面設定12:如第2及4圖所示,二測頭3設置定位後,由二測頭3本身虛擬一位在晶圓2上或下之基準平面R。 Reference Plane Setting 12: As shown in Figures 2 and 4, after the two probes 3 are positioned, the two probes 3 themselves are virtual one bit on the reference plane R on or below the wafer 2.

量測13:如第2及4圖所示,二測頭3之發射器31分別對晶圓2之上表面21和下表面22發射近紅外線光,且由對應之接收器32分別接收從上表面21和下表面22反射之近紅外線光。前述近紅外線光遇有所述透明層時穿透,且在所述透明層之內表面所貼合之上表面21或下表面22及其外表面,皆有反射之近紅外線光被對應之接收器32所接收。 Measurement 13: As shown in Figures 2 and 4, the emitters 31 of the two probes 3 respectively emit near-infrared light to the upper surface 21 and the lower surface 22 of the wafer 2, and are received by the corresponding receivers 32, respectively. The near-infrared light reflected by the surface 21 and the lower surface 22 is. The near-infrared light penetrates when the transparent layer is encountered, and the upper surface 21 or the lower surface 22 and the outer surface thereof are bonded to the inner surface of the transparent layer, and the reflected near-infrared light is received correspondingly. Received by device 32.

計算14:如第3圖所示,有一計算單元4和二測頭3電性連接,晶圓2之上表面21和下表面22以及所述透明層之外表面中,依前述各接收器32所接收之近紅外線光,經計算而獲得和基準平面R間最遠者之距離為一第一距離,和基準平面R間最近者之距離為一第二距離,所述透明層之厚度由其內表面所貼合之上表面21或下表面22及其外表面分別和基準平面R間之距離的差所獲得,以該第一距離減去該第二距離而獲得晶圓2包含該至少一透明層之總厚度,再以該總厚度減去該至少一透明層之厚度而獲得晶圓2本身之厚度。 Calculation 14: As shown in FIG. 3, a computing unit 4 and two probes 3 are electrically connected, the upper surface 21 and the lower surface 22 of the wafer 2, and the outer surface of the transparent layer, according to the foregoing receivers 32. The received near-infrared light is calculated to obtain a distance from the farthest distance between the reference planes R as a first distance, and the closest distance between the reference planes R is a second distance, and the thickness of the transparent layer is determined by the distance The difference between the distance between the upper surface 21 or the lower surface 22 and the outer surface of the inner surface and the reference surface R is respectively obtained by subtracting the second distance from the first distance to obtain the wafer 2 including the at least one The total thickness of the transparent layer is further reduced by the thickness of the at least one transparent layer to obtain the thickness of the wafer 2 itself.

所述各測頭3之發射器31所發射之近紅外線光的波長為850nm為較佳;此外,該總厚度之量測範圍,較佳在50um至2000um。 Preferably, the wavelength of the near-infrared light emitted by the emitter 31 of each of the probes 3 is 850 nm; moreover, the measurement range of the total thickness is preferably 50 um to 2000 um.

在一較佳實施例中,所述至少一透明層,如第2圖所示,有一在晶圓2之下表面22的膠帶層5。於此實施例中,在量測13步驟時,二測頭3之發射器31分別對晶圓2之上表面21和下表面22發射近紅外線光,且由對應之接收器32分別接收從上表面21和下表面22反射之近紅外線光。晶圓2下方之測頭3之發射器31對晶圓2之下表面22發射近紅外線光時,近紅外線光遇膠帶層5穿透,且在膠帶層5之內表面51所貼合之下表面22及其外表面52,皆有反射之近紅外線光被晶圓2下方之測頭3之接收器32所接收。 In a preferred embodiment, the at least one transparent layer, as shown in FIG. 2, has a layer of tape 5 on the lower surface 22 of the wafer 2. In this embodiment, in the step of measuring 13, the emitters 31 of the two probes 3 respectively emit near-infrared light to the upper surface 21 and the lower surface 22 of the wafer 2, and are respectively received by the corresponding receivers 32 from above. The near-infrared light reflected by the surface 21 and the lower surface 22 is. When the emitter 31 of the probe 3 below the wafer 2 emits near-infrared light to the lower surface 22 of the wafer 2, the near-infrared light penetrates through the tape layer 5 and is adhered to the inner surface 51 of the tape layer 5 The surface 22 and its outer surface 52, both of which have reflected near-infrared light, are received by the receiver 32 of the probe 3 below the wafer 2.

承上,在計算14步驟時,本實施例在晶圓2之上表面21和基準平面R間距離最遠而為一第一距離D1,本實施例在膠帶層5之外表面52和基準平面R間距離最近而為一第二距離D2,膠帶層5之內表面51所貼合之下表面22和基準平面R間為一第三距離D3。於此,膠帶層5之厚度T1即第三距離D3減第二距離D2的差所獲得,以第一距離D1減去第二距離D2而獲得晶圓2包含膠帶層5之總厚度T,再以總厚度T減去膠帶層5之厚度T1而獲得晶圓2本身之厚度T2。 As a result, in the calculation of the 14 steps, the distance between the upper surface 21 of the wafer 2 and the reference plane R is the farthest distance and is a first distance D1. The outer surface 52 and the reference plane of the tape layer 5 in this embodiment. The distance between R is the closest to a second distance D2, and the surface 22 between the lower surface 51 of the tape layer 5 and the reference plane R is a third distance D3. Here, the thickness T1 of the tape layer 5 is obtained by subtracting the difference between the third distance D3 and the second distance D2, and the second distance D2 is subtracted from the first distance D1 to obtain the total thickness T of the wafer 2 including the tape layer 5, and then The thickness T2 of the wafer 2 itself is obtained by subtracting the thickness T1 of the tape layer 5 from the total thickness T.

另一較佳實施例中,所述至少一透明層,如第4圖所示,包括前述在晶圓2之下表面22的膠帶層5,另有一在晶圓2之上表面21的保護層6,此保護層6為一種鍍膜。於此實施例中,在量測13步驟時,二測頭3之發射器31同樣分別對晶圓2之上表面21和下表面22發射近紅外線光,且由對應之接收器32分別接收從上表面21和下表面22反射之近紅外線光。晶圓2上方之測頭3之發射器31對晶圓2之上表面21發射近紅外線光時,近紅 外線光遇保護層6穿透,且在保護層6之內表面61所貼合之上表面21及其外表面62,皆有反射之近紅外線光被晶圓2上方之測頭3之接收器32所接收。晶圓2下方之測頭3之發射器31對晶圓2之下表面22發射近紅外線光時,同樣在近紅外線光遇膠帶層5穿透,且在膠帶層5之內表面51所貼合之下表面22及其外表面52,皆有反射之近紅外線光被晶圓2下方之測頭3之接收器32所接收。 In another preferred embodiment, the at least one transparent layer, as shown in FIG. 4, includes the tape layer 5 on the lower surface 22 of the wafer 2, and a protective layer on the upper surface 21 of the wafer 2. 6. The protective layer 6 is a plating film. In this embodiment, in the step of measuring 13, the emitters 31 of the two probes 3 also respectively emit near-infrared light to the upper surface 21 and the lower surface 22 of the wafer 2, and are respectively received by the corresponding receivers 32. The near surface 21 and the lower surface 22 reflect near-infrared light. When the emitter 31 of the probe 3 above the wafer 2 emits near-infrared light to the upper surface 21 of the wafer 2, the near red The external light is penetrated by the protective layer 6, and the upper surface 21 and the outer surface 62 of the inner surface 61 of the protective layer 6 are covered by the receiver of the probe 3 which is reflected by the near-infrared light above the wafer 2. 32 received. When the emitter 31 of the probe 3 below the wafer 2 emits near-infrared light to the lower surface 22 of the wafer 2, it also penetrates the tape layer 5 in the near-infrared light, and is bonded to the inner surface 51 of the tape layer 5. The lower surface 22 and its outer surface 52, both of which have reflected near-infrared light, are received by the receiver 32 of the probe 3 below the wafer 2.

承上,在計算14步驟時,本實施例在保護層6之外表面62和基準平面R間距離最遠而為一第一距離d1,本實施例在膠帶層5之外表面52和基準平面R間距離最近而為一第二距離d2,膠帶層5之內表面51所貼合之下表面22和基準平面R間為一第三距離d3,保護層6之內表面61所貼合之上表面21和基準平面R間為一第四距離d4。於此,膠帶層5之厚度t1即第三距離D3減第二距離D2的差所獲得,保護層6之厚度t2即第一距離d1減第四距離d4的差所獲得,以第一距離d1減去第二距離d2而獲得晶圓2包含膠帶層5和保護層6之總厚度t,再以總厚度t減去膠帶層5之厚度t1和保護層6之厚度t2,以獲得晶圓2本身之厚度t3。 In the calculation step 14, the distance between the outer surface 62 of the protective layer 6 and the reference plane R is the farthest distance of the present embodiment and is a first distance d1. The outer surface 52 and the reference plane of the tape layer 5 in this embodiment. The distance between R is the second distance d2, and the inner surface 51 of the tape layer 5 is a third distance d3 between the surface 22 and the reference plane R. The inner surface 61 of the protective layer 6 is attached. Between the surface 21 and the reference plane R is a fourth distance d4. Here, the thickness t1 of the tape layer 5 is obtained by the difference between the third distance D3 and the second distance D2, and the thickness t2 of the protective layer 6 is obtained by the difference between the first distance d1 and the fourth distance d4, and the first distance d1 is obtained. Subtracting the second distance d2 to obtain the total thickness t of the wafer 2 including the tape layer 5 and the protective layer 6, and subtracting the thickness t1 of the tape layer 5 and the thickness t2 of the protective layer 6 by the total thickness t to obtain the wafer 2 Its thickness is t3.

由上述之說明不難發現本發明之優點在於,即使晶圓2在磊晶過程而在上表面21或下表面22形成如前所述之金屬表面,仍可藉由二測頭3設置近紅外線光之發射器31和接收器32,透過發射器31所發射之近紅外線光在上表面21、下表面22以及所述透明層之外表面反射後被對應的接收器32所接收,並透過前述計算單元4在計算4步驟中獲得各表面和基準平面R間的距離,即可透過相減而獲得晶圓2包含透明層的總厚度,以及該 總厚度減去透明層之厚度所獲得晶圓2本身之厚度,而可達到量測晶圓厚度之精確性和便利性。 From the above description, it is not difficult to find that the present invention is advantageous in that even if the wafer 2 is formed into the metal surface as described above on the upper surface 21 or the lower surface 22 during the epitaxial process, the near infrared rays can be disposed by the two probes 3. The light emitter 31 and the receiver 32 are reflected by the near-infrared light emitted by the emitter 31 on the upper surface 21, the lower surface 22 and the outer surface of the transparent layer, and are received by the corresponding receiver 32, and transmitted through the foregoing The calculating unit 4 obtains the distance between each surface and the reference plane R in the calculation step 4, that is, the total thickness of the wafer 2 including the transparent layer is obtained through subtraction, and the The thickness of the wafer 2 itself is obtained by subtracting the thickness of the transparent layer from the total thickness, and the accuracy and convenience of measuring the thickness of the wafer can be achieved.

以上所述實施例之揭示係用以說明本發明,並非用以限制本發明,故舉凡數值之變更或等效元件之置換仍應隸屬本發明之範疇。 The above description of the embodiments is intended to be illustrative of the invention and is not intended to limit the scope of the invention.

由以上詳細說明,可使熟知本項技藝者明瞭本發明的確可達成前述目的,實已符合專利法之規定,爰提出專利申請。 From the above detailed description, it will be apparent to those skilled in the art that the present invention can achieve the foregoing objects and is in accordance with the provisions of the Patent Law.

Claims (5)

一種運用近紅外線量測晶圓厚度之方法,前述晶圓以水平設置而有一上表面和一下表面,該上表面和該下表面皆不為近紅外線光所能穿透,且該上表面和該下表面之至少一者有透明層,所述透明層有一和該上表面或該下表面貼合之內表面,且有一背對該內表面之外表面,該方法包括以下步驟: 設置測頭:有二測頭分別設在該晶圓的上方和下方,該二測頭各有一組對應的發射器和接收器,該二測頭之發射器可分別對該晶圓之上表面和下表面發射近紅外線光,且由對應之接收器接收反射之近紅外線光; 基準平面設定:該二測頭設置定位後,由該二測頭本身虛擬一位在該晶圓上或下之基準平面; 量測:該二測頭之發射器分別對該晶圓之上、下表面發射近紅外線光,且由對應之接收器分別接收從該上、下表面反射之近紅外線光;前述近紅外線光遇有所述透明層時穿透,且在所述透明層之內表面所貼合之該上表面或該下表面及其外表面,皆有反射之近紅外線光被對應之接收器所接收; 計算:有一計算單元和該二測頭電性連接,該晶圓之上表面和下表面以及所述透明層之外表面中,依前述各接收器所接收之近紅外線光經計算而獲得和該基準平面間最遠者之距離為一第一距離,和該基準平面間最近者之距離為一第二距離,所述透明層之厚度由其內表面所貼合之該上表面或該下表面及其外表面分別和該基準平面間之距離的差所獲得,以該第一距離減去該第二距離而獲得該晶圓包含該至少一透明層之總厚度,再以該總厚度減去該至少一透明層之厚度而獲得該晶圓本身之厚度。A method for measuring a wafer thickness by using a near-infrared ray, wherein the wafer is horizontally disposed to have an upper surface and a lower surface, the upper surface and the lower surface are not penetrated by near-infrared light, and the upper surface and the upper surface At least one of the lower surfaces has a transparent layer, the transparent layer has an inner surface that conforms to the upper surface or the lower surface, and has an outer surface facing away from the inner surface, the method comprising the steps of: arranging the probe: Two probes are respectively disposed above and below the wafer, and each of the two probes has a corresponding set of transmitters and receivers, and the emitters of the two probes respectively emit the upper surface and the lower surface of the wafer Near-infrared light, and receiving reflected near-infrared light by the corresponding receiver; reference plane setting: after the two probes are positioned, the two probes themselves virtualize a reference plane on or under the wafer; The emitters of the two probes respectively emit near-infrared light on the upper and lower surfaces of the wafer, and the corresponding receivers respectively receive near-infrared light reflected from the upper and lower surfaces; the near-infrared When the light encounters the transparent layer, the upper surface or the lower surface and the outer surface of the inner surface of the transparent layer are covered, and the reflected near-infrared light is received by the corresponding receiver. Calculating: a computing unit and the two probes are electrically connected, and the upper surface and the lower surface of the wafer and the outer surface of the transparent layer are obtained by calculation according to the near-infrared light received by the foregoing receivers. The farthest distance between the reference planes is a first distance, and the closest distance between the reference planes is a second distance, and the thickness of the transparent layer is the upper surface or the lower surface to which the inner surface is attached Obtaining a difference between a distance between the surface and the outer surface thereof and the reference plane, and subtracting the second distance from the first distance to obtain a total thickness of the wafer including the at least one transparent layer, and then subtracting the total thickness The thickness of the at least one transparent layer is obtained to obtain the thickness of the wafer itself. 依請求項1所述之運用近紅外線量測晶圓厚度之方法,其中,所述至少一透明層,有一在該晶圓之下表面的膠帶層。A method for measuring a wafer thickness using near infrared ray according to claim 1, wherein the at least one transparent layer has a tape layer on a lower surface of the wafer. 依請求項2所述之運用近紅外線量測晶圓厚度之方法,其中,所述至少一透明層,另有一在該晶圓之上表面的保護層。The method of measuring the thickness of a wafer by using near infrared ray according to claim 2, wherein the at least one transparent layer has a protective layer on the upper surface of the wafer. 依請求項1所述之運用近紅外線量測晶圓厚度之方法,其中,各該測頭之發射器所發射之近紅外線光的波長為850nm。The method for measuring the thickness of a wafer by using near-infrared light according to claim 1, wherein the wavelength of the near-infrared light emitted by the emitter of each of the probes is 850 nm. 依請求項1所述之運用近紅外線量測晶圓厚度之方法,其中,該總厚度之量測範圍在50um至2000um。The method of measuring the thickness of a wafer by using near infrared ray according to claim 1, wherein the total thickness is measured in a range of 50 um to 2000 um.
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